Communication pubs.acs.org/IC
Correlation of the Electronic and Geometric Structures in Mononuclear Copper(II) Superoxide Complexes Jake W. Ginsbach,† Ryan L. Peterson,‡ Ryan E. Cowley,† Kenneth D. Karlin,*,‡ and Edward I. Solomon*,† †
Department of Chemistry, Stanford University, Stanford, California 94305, United States Department of Chemistry, Johns Hopkins University, Baltimore, Maryland 21218, United States
‡
S Supporting Information *
ABSTRACT: The geometry of mononuclear copper(II) superoxide complexes has been shown to determine their ground state where side-on bonding leads to a singlet ground state and end-on complexes have triplet ground states. In an apparent contrast to this trend, the recently synthesized (HIPT3tren)CuIIO2•− (1) was proposed to have an end-on geometry and a singlet ground state. However, reexamination of 1 with resonance Raman, magnetic circular dichroism, and 2H NMR spectroscopies indicate that 1 is, in fact, an end-on superoxide species with a triplet ground state that results from the single CuIIO2•− bonding interaction being weaker than the spinpairing energy. Figure 1. Molecular orbital diagrams of side-on (left) and end-on (right) copper(II) superoxide bonding.
T
he activation of dioxygen at a single copper(I) site to produce a copper(II) superoxide species appears to be essential for the enzymatic function of the noncoupled binuclear copper monooxygenases (PHM, DβM, and TβM)1 and has been recently proposed for the copper-dependent polysaccharide monooxygenases.2 Because isolation of a discrete copper(II) superoxide species in enzymatic systems has been limited to a crystal structure of PHM,1c insight into the electronic structure and bonding in copper(II) superoxide species has been derived from model complexes. In these synthetic complexes, two structures have been observed: superoxide coordinated to copper(II) in a side-on (η2) or end-on (η1) binding mode. The side-on superoxide species, structurally characterized in a tris(pyrazolyl)borate model complex,3 has an O−O stretching frequency of 1043 cm−1 and a copper(II) X-ray absorption pre-edge feature at ∼8979 eV.4 Magnetic susceptibility measurements indicated that the side-on superoxide has a singlet ground state.4a This ground state is a direct result of the two strong Cu−O bonds of the side-on geometry (1.84 Å), causing the highest occupied molecular orbital (HOMO)/lowest unoccupied molecular orbital (LUMO) splitting to be larger than the spin-pairing energy.4a This results in a doubly occupied HOMO that is a superoxidebased π* orbital that is vertical to the Cu−O2 plane (π*v) and an empty Cu dx2−y2 LUMO that is antibonding with the filled π* orbital, forming a very covalent σ bond with the copper (π*σ + αd; Figure 1, left). An end-on superoxide species, which has been structurally characterized in (TMG3tren)CuIIO2•− (TMG = tetramethylguanidino),5 shares similar superoxide spectral features with the side-on complex (νO−O of 1120 cm−1).6 However, both NMR7 © 2013 American Chemical Society
and variable-temperature variable-field magnetic circular dichroism (VTVH-MCD)6b spectroscopies indicate that the end-on superoxide possesses a triplet ground state, in contrast to the singlet ground state of the side-on isomer.4a For the end-on superoxide, the single Cu−O bond (1.93 Å)5 is significantly weaker than the two bonds in the side-on complex, and hence the bonding/antibonding interaction between the superoxide π*σ and the Cu d orbital is unable to overcome the spin-pairing energy.6b This results in a triplet ground state with two singly occupied, orthogonal orbitals: a superoxide π*v orbital and a Cu dz2 orbital (that is, antibonding with the π*σ orbital; Figure 1, right). Recently, Itoh and co-workers synthesized an end-on superoxide adduct 1,8 (HIPT3tren)CuIIO2•− (HIPT = hexaisopropylterphenyl; Scheme 1), which features the same tren ligand platform in (TMG3tren)CuIIO2•−. Although 1 has vibrational features similar to those of (TMG3tren)CuIIO2•− [νO−O = 1095 cm−1 from rR excitation into the O2•− → CuII charge transfer (CT) at 23000 cm−1], they proposed that 1 has a singlet ground Scheme 1. (HIPT3tren)CuIIO2•− Complex 1
Received: September 17, 2013 Published: October 28, 2013 12872
dx.doi.org/10.1021/ic402357u | Inorg. Chem. 2013, 52, 12872−12874
Inorganic Chemistry
Communication
state due to the observation of chemical shifts between 8 and 0 ppm in its 1H NMR spectrum.8 This intriguing result prompted us to probe the electronic structure of 1 in the context of the endon triplet/side-on singlet correlation described in Figure 1. To probe the geometric structure of 1, resonance Raman (rR) spectra were collected on samples prepared with 16O2, 18O2, and a 16O−18O mixed isotope dioxygen (16,18O2; Figure S1 in the Supporting Information, SI). Two νCu−O were observed in the 16,18 O2 spectrum that have the same energy as νCu−O in the 16O2 and 18O2 spectra, indicating an asymmetric (i.e., end-on) coordination mode of superoxide.9 The ground state and electronic structure of 1 were then probed with VTVH-MCD spectroscopy. A 9:1 mixture of n-propanol and acetone was selected as an appropriate solvent because it formed an optical glass without affecting the absorption (Abs) or rR spectra of 1 (Figures S1 and S2 in the SI). The Abs and low-temperature (5.0 K) MCD spectra of oxygenated samples of (HIPT3tren)CuI require five Gaussian bands to fit both experimental spectra up to and including the O2•− → CuII CT transition (band 5; Figure 2 and Table S1 in the
Figure 3. VTVH-MCD isotherms and fit (D = +3.0 and E/D = 0.17) for band 2 collected at 14040 cm−1.
spectroscopy. Therefore, the NMR spectroscopy of 1 was reexamined. The 1H NMR spectra of oxygen-saturated samples of (HIPT3tren)CuI in acetone were indistinguishable from the original (HIPT3tren)CuI at 183 K (−90 °C; Figure S7 in the SI). However, the previously determined equilibrium constant for O2 binding (Keq = 0.11 mM−1) 8 indicates that 1 is only approximately half-oxygenated under these conditions ([Cu]0 11 = 3.0 mM, [O2]0 ≈ 14 mM ). Because no new chemical shifts were initially observed in the 1H NMR spectra, deuterium was incorporated into a single position on each HIPT substituent (see Scheme 1). 2H NMR spectra of oxygen-saturated samples of (d3-HIPT3tren)CuI show two resonances with approximately equal intensity: one corresponding to (d3-HIPT3tren)CuI and a new paramagnetically shifted resonance at −24 ppm (Figure 4),
Figure 2. Absorption (183 K, top) and MCD (5.0 K, bottom) spectra of 1 and Gaussian fits. Band 0 (*) indicates an S = 1/2 contaminant.
SI). Agreement between the transition energies in both spectra indicates that the MCD intensity in these bands can be assigned to 1. The MCD spectrum of 1 is also similar to that previously obtained for (TMG3tren)CuIIO2•−:6b a derivative-shaped pseudo-A (bands 2 and 3), a negative transition to higher energy (band 4), and a positive transition resulting from the O2•− → CuII CT transition (band 5). However, bands 2−4 are shifted up in energy by >3000 cm−1 in 1 relative to (TMG3tren)CuIIO2•−, indicating that HIPT3tren possesses a weaker ligand field.6b An additional band (band 0) is required to fit the lowest-energy feature in the MCD spectrum. While the relative intensity of bands 1−5 were constant between multiple samples, the intensity of band 0 was variable (Figure S3 in the SI) and is assigned as an S = 1/2 contaminant because its VTVH-MCD isotherms overlay (Figure S4 in the SI). In contrast, VTVHMCD isotherms collected on bands 1−4 (Figures 3 and S5 in the SI) show nonoverlapping (nesting) behavior, which results from zero-field splitting (ZFS). This ZFS requires that 1 has an S > 1/2 ground state. The saturation magnetization curves for bands 1−5 fit to the spin Hamiltonian for an S = 1 system with axial (D) and rhombic (E) zero-field parameters of D = +3.0 and 0.22 ≥ E/D ≥ 0.12 (see the SI for details). While the nesting observed in the VTVH-MCD isotherms requires 1 to have a paramagnetic ground state (S = 1), ref 8 reported the ground state to be diamagnetic (S = 0) from NMR
Figure 4. 2H NMR spectra of 3 mM d3-HIPT3tren derivatives in acetone at 183 K (−90 °C): CuI (gold, 7.3 ppm), CuIIO2•− (1) (green, 7.3 and −24 ppm), and CuICO (black, 7.4 ppm). # indicates d12-SiMe4 (0 ppm) and * natural abundance deuterium in acetone (2.05 ppm).
which is assigned to 1. The addition of CO to 1 resulted in a single chemical shift corresponding to (d3-HIPT3tren)CuICO, indicating that the resonance at −24 ppm did not arise from an S = 1/2 contaminant. Reanalysis of the 1H NMR spectra indicated the presence of a broad, weak resonance at −24 ppm (Figures S7 and S8 in the SI). Similarly, density functional theory (DFT) calculations on a truncated model of 1 predict a triplet ground state, with both closed-shell singlet (+23.2 kcal/mol) and broken-symmetry singlet (+13.0 kcal/mol) states at significantly higher energy (Figures S9 and S10 and Tables S3 and S4 in the SI), in agreement with the experimental data presented above. In summary, rR spectroscopy with mixed isotope dioxygen confirms the end-on superoxide geometry of 1, while VTVHMCD and NMR spectroscopies determine that 1 has a triplet ground state. While the Cu−O bond in 1 is stronger than that in (TMG3tren)CuIIO2•−, this single Cu−O bond is unable to overcome the pairing energy required to form a singlet ground state (Figure 1). To date, only a side-on superoxide complex with two Cu−O bonds has the required bond strength to overcome 12873
dx.doi.org/10.1021/ic402357u | Inorg. Chem. 2013, 52, 12872−12874
Inorganic Chemistry
Communication
the spin-pairing energy resulting in a singlet ground state.4a These results suggest that the end-on superoxide intermediate proposed in the enzymatic systems1c should also have a triplet ground state. This prediction awaits experimental evaluation.
■
ASSOCIATED CONTENT
S Supporting Information *
Additional synthetic details, rR, Abs, VTVH-MCD, NMR, and DFT calculations. This material is available free of charge via the Internet at http://pubs.acs.org.
■
AUTHOR INFORMATION
Corresponding Authors
*E-mail: [email protected]. *E-mail: [email protected]. Notes
The authors declare no competing financial interest.
■
ACKNOWLEDGMENTS This research was supported by NIH Grants DK31450 (to E.I.S.), GM28962 (to K.D.K.), and a Ruth L. Kirschstein National Research Service Award F32-GM105288 (to R.E.C.).
■
REFERENCES
(1) (a) Evans, J. P.; Ahn, K.; Klinman, J. P. J. Biol. Chem. 2003, 278, 49691. (b) Chen, P.; Bell, J.; Eipper, B. A.; Solomon, E. I. Biochemistry 2004, 43, 5735. (c) Prigge, S. T.; Eipper, B. A.; Mains, R. E.; Amzel, L. M. Science 2004, 304, 864. (2) Phillips, C. M.; Beeson, W. T. I. V.; Cate, J. H.; Marletta, M. A. ACS Chem. Biol. 2011, 6, 1399. (3) Fujisawa, K.; Tanaka, M.; Moro-oka, Y.; Kitajima, N. J. Am. Chem. Soc. 1994, 116, 12079. (4) (a) Chen, P.; Root, D. E.; Campochiaro, C.; Fujisawa, K.; Solomon, E. I. J. Am. Chem. Soc. 2003, 125, 466. (b) Sarangi, R.; Aboelella, N.; Fujisawa, K.; Tolman, W. B.; Hedman, B.; Hodgson, K. O.; Solomon, E. I. J. Am. Chem. Soc. 2006, 128, 8286. (5) Würtele, C.; Gaoutchenova, E.; Harms, K.; Holthausen, M. C.; Sundermeyer, J.; Schindler, S. Angew. Chem., Int. Ed. 2006, 45, 3867. (6) (a) Schatz, M.; Raab, V.; Foxon, S. P.; Brehm, G.; Schneider, S.; Reiher, M.; Holthausen, M. C.; Sundermeyer, J.; Schindler, S. Angew. Chem., Int. Ed. 2004, 43, 4360. (b) Woertink, J. S.; Tian, L.; Maiti, D.; Lucas, H. R.; Himes, R. A.; Karlin, K. D.; Neese, F.; Würtele, C.; Holthausen, M. C.; Bill, E.; Sundermeyer, J.; Schindler, S.; Solomon, E. I. Inorg. Chem. 2010, 49, 9450. (7) Lanci, M. P.; Roth, J. P. J. Am. Chem. Soc. 2006, 128, 16006. (8) Kobayashi, Y.; Ohkubo, K.; Nomura, T.; Kubo, M.; Fujieda, N.; Sugimoto, H.; Fukuzumi, S.; Goto, K.; Ogura, T.; Itoh, S. Eur. J. Inorg. Chem. 2012, 29, 4574. (9) A single νCu−O at intermediate energy would be expected from a symmetric (i.e., side-on) coordination mode.10 (10) Maiti, D.; Fry, H. C.; Woertink, J. S.; Vance, M. A.; Solomon, E. I.; Karlin, K. D. J. Am. Chem. Soc. 2007, 129, 264−265. (11) Kretschmer, C. B.; Nowakowska, J.; Wiebe, R. Ind. Eng. Chem. 1946, 38, 506.
12874
dx.doi.org/10.1021/ic402357u | Inorg. Chem. 2013, 52, 12872−12874
Correlation of the Electronic and Geometric Structures in Mononuclear Copper(II) Superoxide Complexes Jake W. Ginsbach,† Ryan L. Peterson,‡ Ryan E. Cowley,† Kenneth D. Karlin,*,‡ and Edward I. Solomon*,† †
Department of Chemistry, Stanford University, Stanford, California 94305, United States Department of Chemistry, Johns Hopkins University, Baltimore, Maryland 21218, United States
‡
S Supporting Information *
ABSTRACT: The geometry of mononuclear copper(II) superoxide complexes has been shown to determine their ground state where side-on bonding leads to a singlet ground state and end-on complexes have triplet ground states. In an apparent contrast to this trend, the recently synthesized (HIPT3tren)CuIIO2•− (1) was proposed to have an end-on geometry and a singlet ground state. However, reexamination of 1 with resonance Raman, magnetic circular dichroism, and 2H NMR spectroscopies indicate that 1 is, in fact, an end-on superoxide species with a triplet ground state that results from the single CuIIO2•− bonding interaction being weaker than the spinpairing energy. Figure 1. Molecular orbital diagrams of side-on (left) and end-on (right) copper(II) superoxide bonding.
T
he activation of dioxygen at a single copper(I) site to produce a copper(II) superoxide species appears to be essential for the enzymatic function of the noncoupled binuclear copper monooxygenases (PHM, DβM, and TβM)1 and has been recently proposed for the copper-dependent polysaccharide monooxygenases.2 Because isolation of a discrete copper(II) superoxide species in enzymatic systems has been limited to a crystal structure of PHM,1c insight into the electronic structure and bonding in copper(II) superoxide species has been derived from model complexes. In these synthetic complexes, two structures have been observed: superoxide coordinated to copper(II) in a side-on (η2) or end-on (η1) binding mode. The side-on superoxide species, structurally characterized in a tris(pyrazolyl)borate model complex,3 has an O−O stretching frequency of 1043 cm−1 and a copper(II) X-ray absorption pre-edge feature at ∼8979 eV.4 Magnetic susceptibility measurements indicated that the side-on superoxide has a singlet ground state.4a This ground state is a direct result of the two strong Cu−O bonds of the side-on geometry (1.84 Å), causing the highest occupied molecular orbital (HOMO)/lowest unoccupied molecular orbital (LUMO) splitting to be larger than the spin-pairing energy.4a This results in a doubly occupied HOMO that is a superoxidebased π* orbital that is vertical to the Cu−O2 plane (π*v) and an empty Cu dx2−y2 LUMO that is antibonding with the filled π* orbital, forming a very covalent σ bond with the copper (π*σ + αd; Figure 1, left). An end-on superoxide species, which has been structurally characterized in (TMG3tren)CuIIO2•− (TMG = tetramethylguanidino),5 shares similar superoxide spectral features with the side-on complex (νO−O of 1120 cm−1).6 However, both NMR7 © 2013 American Chemical Society
and variable-temperature variable-field magnetic circular dichroism (VTVH-MCD)6b spectroscopies indicate that the end-on superoxide possesses a triplet ground state, in contrast to the singlet ground state of the side-on isomer.4a For the end-on superoxide, the single Cu−O bond (1.93 Å)5 is significantly weaker than the two bonds in the side-on complex, and hence the bonding/antibonding interaction between the superoxide π*σ and the Cu d orbital is unable to overcome the spin-pairing energy.6b This results in a triplet ground state with two singly occupied, orthogonal orbitals: a superoxide π*v orbital and a Cu dz2 orbital (that is, antibonding with the π*σ orbital; Figure 1, right). Recently, Itoh and co-workers synthesized an end-on superoxide adduct 1,8 (HIPT3tren)CuIIO2•− (HIPT = hexaisopropylterphenyl; Scheme 1), which features the same tren ligand platform in (TMG3tren)CuIIO2•−. Although 1 has vibrational features similar to those of (TMG3tren)CuIIO2•− [νO−O = 1095 cm−1 from rR excitation into the O2•− → CuII charge transfer (CT) at 23000 cm−1], they proposed that 1 has a singlet ground Scheme 1. (HIPT3tren)CuIIO2•− Complex 1
Received: September 17, 2013 Published: October 28, 2013 12872
dx.doi.org/10.1021/ic402357u | Inorg. Chem. 2013, 52, 12872−12874
Inorganic Chemistry
Communication
state due to the observation of chemical shifts between 8 and 0 ppm in its 1H NMR spectrum.8 This intriguing result prompted us to probe the electronic structure of 1 in the context of the endon triplet/side-on singlet correlation described in Figure 1. To probe the geometric structure of 1, resonance Raman (rR) spectra were collected on samples prepared with 16O2, 18O2, and a 16O−18O mixed isotope dioxygen (16,18O2; Figure S1 in the Supporting Information, SI). Two νCu−O were observed in the 16,18 O2 spectrum that have the same energy as νCu−O in the 16O2 and 18O2 spectra, indicating an asymmetric (i.e., end-on) coordination mode of superoxide.9 The ground state and electronic structure of 1 were then probed with VTVH-MCD spectroscopy. A 9:1 mixture of n-propanol and acetone was selected as an appropriate solvent because it formed an optical glass without affecting the absorption (Abs) or rR spectra of 1 (Figures S1 and S2 in the SI). The Abs and low-temperature (5.0 K) MCD spectra of oxygenated samples of (HIPT3tren)CuI require five Gaussian bands to fit both experimental spectra up to and including the O2•− → CuII CT transition (band 5; Figure 2 and Table S1 in the
Figure 3. VTVH-MCD isotherms and fit (D = +3.0 and E/D = 0.17) for band 2 collected at 14040 cm−1.
spectroscopy. Therefore, the NMR spectroscopy of 1 was reexamined. The 1H NMR spectra of oxygen-saturated samples of (HIPT3tren)CuI in acetone were indistinguishable from the original (HIPT3tren)CuI at 183 K (−90 °C; Figure S7 in the SI). However, the previously determined equilibrium constant for O2 binding (Keq = 0.11 mM−1) 8 indicates that 1 is only approximately half-oxygenated under these conditions ([Cu]0 11 = 3.0 mM, [O2]0 ≈ 14 mM ). Because no new chemical shifts were initially observed in the 1H NMR spectra, deuterium was incorporated into a single position on each HIPT substituent (see Scheme 1). 2H NMR spectra of oxygen-saturated samples of (d3-HIPT3tren)CuI show two resonances with approximately equal intensity: one corresponding to (d3-HIPT3tren)CuI and a new paramagnetically shifted resonance at −24 ppm (Figure 4),
Figure 2. Absorption (183 K, top) and MCD (5.0 K, bottom) spectra of 1 and Gaussian fits. Band 0 (*) indicates an S = 1/2 contaminant.
SI). Agreement between the transition energies in both spectra indicates that the MCD intensity in these bands can be assigned to 1. The MCD spectrum of 1 is also similar to that previously obtained for (TMG3tren)CuIIO2•−:6b a derivative-shaped pseudo-A (bands 2 and 3), a negative transition to higher energy (band 4), and a positive transition resulting from the O2•− → CuII CT transition (band 5). However, bands 2−4 are shifted up in energy by >3000 cm−1 in 1 relative to (TMG3tren)CuIIO2•−, indicating that HIPT3tren possesses a weaker ligand field.6b An additional band (band 0) is required to fit the lowest-energy feature in the MCD spectrum. While the relative intensity of bands 1−5 were constant between multiple samples, the intensity of band 0 was variable (Figure S3 in the SI) and is assigned as an S = 1/2 contaminant because its VTVH-MCD isotherms overlay (Figure S4 in the SI). In contrast, VTVHMCD isotherms collected on bands 1−4 (Figures 3 and S5 in the SI) show nonoverlapping (nesting) behavior, which results from zero-field splitting (ZFS). This ZFS requires that 1 has an S > 1/2 ground state. The saturation magnetization curves for bands 1−5 fit to the spin Hamiltonian for an S = 1 system with axial (D) and rhombic (E) zero-field parameters of D = +3.0 and 0.22 ≥ E/D ≥ 0.12 (see the SI for details). While the nesting observed in the VTVH-MCD isotherms requires 1 to have a paramagnetic ground state (S = 1), ref 8 reported the ground state to be diamagnetic (S = 0) from NMR
Figure 4. 2H NMR spectra of 3 mM d3-HIPT3tren derivatives in acetone at 183 K (−90 °C): CuI (gold, 7.3 ppm), CuIIO2•− (1) (green, 7.3 and −24 ppm), and CuICO (black, 7.4 ppm). # indicates d12-SiMe4 (0 ppm) and * natural abundance deuterium in acetone (2.05 ppm).
which is assigned to 1. The addition of CO to 1 resulted in a single chemical shift corresponding to (d3-HIPT3tren)CuICO, indicating that the resonance at −24 ppm did not arise from an S = 1/2 contaminant. Reanalysis of the 1H NMR spectra indicated the presence of a broad, weak resonance at −24 ppm (Figures S7 and S8 in the SI). Similarly, density functional theory (DFT) calculations on a truncated model of 1 predict a triplet ground state, with both closed-shell singlet (+23.2 kcal/mol) and broken-symmetry singlet (+13.0 kcal/mol) states at significantly higher energy (Figures S9 and S10 and Tables S3 and S4 in the SI), in agreement with the experimental data presented above. In summary, rR spectroscopy with mixed isotope dioxygen confirms the end-on superoxide geometry of 1, while VTVHMCD and NMR spectroscopies determine that 1 has a triplet ground state. While the Cu−O bond in 1 is stronger than that in (TMG3tren)CuIIO2•−, this single Cu−O bond is unable to overcome the pairing energy required to form a singlet ground state (Figure 1). To date, only a side-on superoxide complex with two Cu−O bonds has the required bond strength to overcome 12873
dx.doi.org/10.1021/ic402357u | Inorg. Chem. 2013, 52, 12872−12874
Inorganic Chemistry
Communication
the spin-pairing energy resulting in a singlet ground state.4a These results suggest that the end-on superoxide intermediate proposed in the enzymatic systems1c should also have a triplet ground state. This prediction awaits experimental evaluation.
■
ASSOCIATED CONTENT
S Supporting Information *
Additional synthetic details, rR, Abs, VTVH-MCD, NMR, and DFT calculations. This material is available free of charge via the Internet at http://pubs.acs.org.
■
AUTHOR INFORMATION
Corresponding Authors
*E-mail: [email protected]. *E-mail: [email protected]. Notes
The authors declare no competing financial interest.
■
ACKNOWLEDGMENTS This research was supported by NIH Grants DK31450 (to E.I.S.), GM28962 (to K.D.K.), and a Ruth L. Kirschstein National Research Service Award F32-GM105288 (to R.E.C.).
■
REFERENCES
(1) (a) Evans, J. P.; Ahn, K.; Klinman, J. P. J. Biol. Chem. 2003, 278, 49691. (b) Chen, P.; Bell, J.; Eipper, B. A.; Solomon, E. I. Biochemistry 2004, 43, 5735. (c) Prigge, S. T.; Eipper, B. A.; Mains, R. E.; Amzel, L. M. Science 2004, 304, 864. (2) Phillips, C. M.; Beeson, W. T. I. V.; Cate, J. H.; Marletta, M. A. ACS Chem. Biol. 2011, 6, 1399. (3) Fujisawa, K.; Tanaka, M.; Moro-oka, Y.; Kitajima, N. J. Am. Chem. Soc. 1994, 116, 12079. (4) (a) Chen, P.; Root, D. E.; Campochiaro, C.; Fujisawa, K.; Solomon, E. I. J. Am. Chem. Soc. 2003, 125, 466. (b) Sarangi, R.; Aboelella, N.; Fujisawa, K.; Tolman, W. B.; Hedman, B.; Hodgson, K. O.; Solomon, E. I. J. Am. Chem. Soc. 2006, 128, 8286. (5) Würtele, C.; Gaoutchenova, E.; Harms, K.; Holthausen, M. C.; Sundermeyer, J.; Schindler, S. Angew. Chem., Int. Ed. 2006, 45, 3867. (6) (a) Schatz, M.; Raab, V.; Foxon, S. P.; Brehm, G.; Schneider, S.; Reiher, M.; Holthausen, M. C.; Sundermeyer, J.; Schindler, S. Angew. Chem., Int. Ed. 2004, 43, 4360. (b) Woertink, J. S.; Tian, L.; Maiti, D.; Lucas, H. R.; Himes, R. A.; Karlin, K. D.; Neese, F.; Würtele, C.; Holthausen, M. C.; Bill, E.; Sundermeyer, J.; Schindler, S.; Solomon, E. I. Inorg. Chem. 2010, 49, 9450. (7) Lanci, M. P.; Roth, J. P. J. Am. Chem. Soc. 2006, 128, 16006. (8) Kobayashi, Y.; Ohkubo, K.; Nomura, T.; Kubo, M.; Fujieda, N.; Sugimoto, H.; Fukuzumi, S.; Goto, K.; Ogura, T.; Itoh, S. Eur. J. Inorg. Chem. 2012, 29, 4574. (9) A single νCu−O at intermediate energy would be expected from a symmetric (i.e., side-on) coordination mode.10 (10) Maiti, D.; Fry, H. C.; Woertink, J. S.; Vance, M. A.; Solomon, E. I.; Karlin, K. D. J. Am. Chem. Soc. 2007, 129, 264−265. (11) Kretschmer, C. B.; Nowakowska, J.; Wiebe, R. Ind. Eng. Chem. 1946, 38, 506.
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dx.doi.org/10.1021/ic402357u | Inorg. Chem. 2013, 52, 12872−12874
